Final Magnetic Moment0.000 μBCalculated total magnetic moment for the unit cell within the magnetic ordering provided (see below). Typically accurate to the second digit. |
Magnetic OrderingNM |
Formation Energy / Atom-1.786 eVCalculated formation energy from the elements normalized to per atom in the unit cell. |
Energy Above Hull / Atom0.032 eVThe energy of decomposition of this material into the set of most stable materials at this chemical composition, in eV/atom. Stability is tested against all potential chemical combinations that result in the material's composition. For example, a Co2O3 structure would be tested for decomposition against other Co2O3 structures, against Co and O2 mixtures, and against CoO and O2 mixtures. |
Density4.69 g/cm3The calculated bulk crystalline density, typically underestimated due calculated cell volumes overestimated on average by 3% (+/- 6%) |
Decomposes ToLiCoO2 |
Band Gap0.000 eVIn general, band gaps computed with common exchange-correlation functionals such as the LDA and GGA are severely underestimated. Typically the disagreement is reported to be ~50% in the literature. Some internal testing by the Materials Project supports these statements; typically, we find that band gaps are underestimated by ~40%. We additionally find that several known insulators are predicted to be metallic. |
Hermann MauguinFd3m [227] |
HallF 4d 2 3 1d |
Point Groupm3m |
Crystal Systemcubic |
Calculated powder diffraction pattern; note that peak spacings may be affected due to inaccuracies in calculated cell volume, which is typically overestimated on average by 3% (+/- 6%)
A full elastic tensor has not been calculated for this material. Registered users can view statistical-learning-based predictions of this material's bulk and shear moduli.
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material | dissimilarity | Ehull | # of elements |
---|---|---|---|
Ca5Mn4O9 (mp-767184) | 0.1016 | 0.026 | 3 |
LiMoO2 (mp-19338) | 0.1083 | 0.008 | 3 |
LiNiO2 (mp-25592) | 0.1121 | 0.012 | 3 |
LiCuO2 (mp-25372) | 0.0909 | 0.068 | 3 |
LiMnO2 (mp-25539) | 0.1072 | 0.098 | 3 |
Li4Fe3CuO8 (mp-763924) | 0.0736 | 0.037 | 4 |
Li2CrFeO4 (mp-765743) | 0.0797 | 1.013 | 4 |
Li4Fe3NiO8 (mp-769856) | 0.0748 | 0.349 | 4 |
Li4V3CrO8 (mp-776143) | 0.0707 | 0.010 | 4 |
Li4CrFe3O8 (mp-771065) | 0.0793 | 1.519 | 4 |
VO (mp-714885) | 0.2216 | 0.018 | 2 |
PbS (mp-1057015) | 0.2106 | 0.001 | 2 |
KN (mp-1064647) | 0.2138 | 1.464 | 2 |
SrN (mp-1078609) | 0.1959 | 0.438 | 2 |
Sb2Te3 (mp-1080789) | 0.2200 | 0.129 | 2 |
Na6MnNi3(SbO6)2 (mp-1094109) | 0.7088 | 0.005 | 5 |
Hg (mp-982872) | 0.2549 | 0.020 | 1 |
Se (mp-7755) | 0.3060 | 0.181 | 1 |
Te (mp-10654) | 0.2485 | 0.047 | 1 |
Te (mp-105) | 0.2711 | 0.047 | 1 |
P (mp-53) | 0.3370 | 0.144 | 1 |
Explore more synthesis descriptions for materials of composition LiCoO2.
Text computed by synthesisproject.org.
Run TypeGGA+U |
Energy Cutoff520 eV |
# of K-pointsNone |
U ValuesCo: 3.32 eV |
PseudopotentialsVASP PAW: Li_sv Co O |
Final Energy/Atom-5.6950 eV |
Corrected Energy-104.2336 eV
-104.2336 eV = -91.1193 eV (uncorrected energy) - 7.4960 eV (MP Advanced Correction) - 5.6183 eV (MP Anion Correction)
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Displaying lattice parameters for primitive cell; note that calculated cell volumes are typically overestimated on average by 3% (+/- 6%). Note the primitive cell may appear less symmetric than the conventional cell representation (see "Structure Type" selector below the 3d structure)